Abstract

Scalable quantum information processing will require quantum networks of qubits with the ability to coherently transfer quantum states between the desired sender and receiver nodes. Here we propose a scheme to implement a quantum router that can direct quantum states from an input qubit to a preselected output qubit. The path taken by the transferred quantum state is controlled by the state of one or more ancilla qubits. This enables both directed transport between a sender and a number of receiver nodes, and generation of distributed entanglement in the network. We demonstrate the general idea using a two-output setup and discuss how the quantum routing may be expanded to several outputs. We also present a possible realization of our ideas with superconducting circuits.

Highlights

  • We present a possible realization of our ideas with superconducting circuits

  • The transfer of quantum information between different quantum processing units will be an integral part of possible future quantum technology

  • State transfer protocols in such networks typically rely on tuning nearest-neighbor couplings and local fields, either statically or dynamically, in order to maximize the fidelity of moving a quantum state across the network in minimum time

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Summary

Introduction

The transfer of quantum information between different quantum processing units will be an integral part of possible future quantum technology. Since a larger quantum processing unit is likely to consists of several smaller devices or subprocessors, it is crucial to have a quantum routing system for selective high-fidelity state transfer and entanglement sharing between a sender and a distinct receiver in a network This issue has previously been considered in several different contexts, including coupled harmonic systems [24], external flux threading [25], local field adjustments in spin systems [26,27,28,29,30,31], using local periodic field modulation [32] to manipulate tunneling rates [33,34,35,36], and using optimal control techniques at local sites [30].

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Conclusion
SUPERCONDUCTING CIRCUIT IMPLEMENTATION OF THE ROUTER
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Residual coupling between the outputs
Coupling to the input qubit
IMPLEMENTATION OF THREE OUTPUT ROUTER
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